Vibrational Frequencies calculated at HSEh1PBE/STO-3G
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A |
3794 |
3350 |
1.48 |
|
|
|
| 2 |
A |
3542 |
3128 |
5.25 |
|
|
|
| 3 |
A |
1726 |
1524 |
20.13 |
|
|
|
| 4 |
A |
1671 |
1476 |
25.57 |
|
|
|
| 5 |
A |
1270 |
1122 |
31.25 |
|
|
|
| 6 |
A |
1047 |
925 |
11.46 |
|
|
|
| 7 |
A |
659 |
582 |
204.53 |
|
|
|
| 8 |
A |
584 |
516 |
55.71 |
|
|
|
| 9 |
A |
438 |
387 |
35.10 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7365.2 cm
-1
Scaled (by 0.8831) Zero Point Vibrational Energy (zpe) 6504.2 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.102 |
|
|
|
| 2 |
N |
0.025 |
|
|
|
| 3 |
N |
-0.306 |
|
|
|
| 4 |
H |
0.187 |
|
|
|
| 5 |
H |
0.196 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.678 |
0.861 |
1.356 |
2.323 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.792 |
0.206 |
2.082 |
| y |
0.206 |
-15.482 |
0.333 |
| z |
2.082 |
0.333 |
-15.194 |
|
| Traceless |
| | x | y | z |
| x |
0.546 |
0.206 |
2.082 |
| y |
0.206 |
-0.489 |
0.333 |
| z |
2.082 |
0.333 |
-0.057 |
|
| Polar |
| 3z2-r2 | -0.114 |
| x2-y2 | 0.690 |
| xy | 0.206 |
| xz | 2.082 |
| yz | 0.333 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.878 |
-0.127 |
0.119 |
| y |
-0.127 |
1.307 |
0.011 |
| z |
0.119 |
0.011 |
0.578 |
<r2> (average value of r
2) Å
2
| <r2> |
38.021 |
| (<r2>)1/2 |
6.166 |